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The Formation of the First Star in the Universe

The Formation of the First Star in the Universe. Abel, Bryan, Norman 2001 Presented Nov 19, 2009 PHY 689 Galaxy Formation. Initial Conditions. Simulating the birth of the very first star has straightforward requirements: Basic Chemical and Radiative processes Negligible B -fields

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The Formation of the First Star in the Universe

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  1. The Formation of the First Star in the Universe Abel, Bryan, Norman 2001 Presented Nov 19, 2009 PHY 689 Galaxy Formation

  2. Initial Conditions • Simulating the birth of the very first star has straightforward requirements: • Basic Chemical and Radiative processes • Negligible B-fields • No other stars • Given initial conditions

  3. Motivation • Metals in young universe Heavy elements had to have been released and distributed in the IGM within first billion years • Supernova source Only known producers of such metals; massive stars must have been amongst the earliest-formed objects

  4. The Simulation • Following from previous work, • Eulerian structured Adaptive Mesh Refinement • Previous studies traced the evolution of a molecular-cloud like structure Fig 2., Abel, Anninos, Norman, & Zhang 1998

  5. What determines the scale of collapse? • Critical mass for gravitational collapse: Isothermal Bonner-Ebert mass MBE=1.18M☉(cs4/G3/2)Pext-1/2 cs2=dP/dρ = γkBT/μmH • Causes for fragmentation? Study builds on previous results by modeling chemical processes that may affect the growth of high-mass stars in early universe

  6. Mass Scales • Four Characteristic Mass Scales emerge • 7x105M☉ falls onto the pregalactic halo • Temperature drops and molecular hydrogen fraction increases: temperature rises cooling becomes more efficient • 100 solar mass core • At center, 1 solar mass H2 protostar

  7. Accretion Snapshot Fig 3., Abel, Bryan & Norman 2001 Fig 2., Abel, Bryan & Norman 2000

  8. Simulation Overview Fig 1., Abel, Bryan & Norman 2001

  9. Chemo-Thermal Instability • The big question in undertaking this simulation was whether further cooling would cause fragmentation • 3-body H interaction H-+H=H2+e- • No correspondingly large density inhomogeneities are found and fragmentation does not occur

  10. Angular Momentum • Rotational support does not halt collapse • Protostellar gas starts out with little angular momentum to lose • Angular momentum is transported outwards from the inner accreting regions

  11. Magnetic Fields? • Influence of magnetic fields at early times considered negligible • Difference in physics of early fields may account for QCD phase transitions and Electro-weak contributions • Ionized fraction of particles drops rapidly; would be sustained in present day by cosmic ray interaction

  12. Results in brief • This work extended previous studies by simulating molecular formation of H2 via 3-body interaction • Previously was uncertain whether this process would lead to fragmentation of the collapsing cloud • Simulation runs out before final stellar mass is established, unknown how much more of the cloud will accrete • Feedback from forming star may limit further accumulation

  13. In Conclusion • At most one massive metal-free star forms per pregalactic halo • Possibility that all metal-free stars are massive and form in isolation; explains absence of purely metal-free low mass stars in Milky Way • Consequences for galaxy formation: metals, entropy, B-fields and possibly baryon power spectrum perturbation

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